Temperature Control Unit for a Gaseous or Liquid Medium

ABSTRACT

For a temperature control unit for gaseous or liquid medium with a highly dynamic temperature regulation of the medium, the temperature control unit ( 1 ) is designed with a base body ( 2 ) and a cooling body ( 5 ) between which are arranged multiple thermoelectric modules ( 7 ) and with a media line ( 6 ) in the base body ( 2 ), and it is provided that the mass ratio of the thermal storage mass of the cooling body ( 5 ) to the thermal storage mass of the base body ( 2 ) and the media line ( 6 ) arranged therein is in the range of 0.5 to 1, advantageously in the range of 0.7 to 0.8.

The present invention relates to a temperature control unit for temperature control of a gaseous or liquid medium by means of a number of thermoelectric modules which are arranged between a base body and a cooling body and a media line through which the gaseous or liquid medium flows is arranged in the base body.

For accurate measurement of the fuel consumption by an internal consumption engine on a test stand, accurate conditioning of the temperature and pressure of the fuel supplied to the internal combustion engine is necessary. The fuel consumption is often measured using a known Coriolis flow sensor. An example of such a measurement of fuel consumption can be found in US 2014/0123742 A1, which is based on conditioning of liquid fuels. In that application, the temperature of the fuel is regulated with a cooling liquid by means of a heat exchanger. Extreme changes in load cause extreme fluctuations in fuel consumption and in the media temperature of the return flow (input temperature). However, such a heat exchanger is sluggish, allowing only gradual changes in temperature. Thus, the conditioning by means of a heat exchanger that has been described is not suitable for extreme load alternations (changes in input temperature). With the current state of the art, this leads to the result that it is necessary to allow a settling time after such a load reversal. During this period of time, the temperature is not stable and a high-precision measurement is impossible for flow sensors. For operation that is independent of the changes in input temperature, one option is to increase the power density of the heat exchanger, but this is not readily feasible technically and would require a redesign of the heat exchanger, if it were possible at all. If the power density remains the same, this would result in a need for a much larger amount of space. Another possibility might consist of a more aggressive regulation of the heat exchanger, but this in turn would mean greater overshooting and undershooting, and, associated with this, inferior dynamics with respect to possible changes in the target temperature. However, increasing the size of the heat exchanger would also be helpful only in the case of liquids. In the case of gaseous media, a change in flow would immediately cause a change in pressure and a change in target temperature. The heat exchanger would therefore have to enable extremely fast changes in target temperature but this cannot be achieved in practical terms for a heat exchanger operated with a cooling liquid. To do so, the available power would have to be further increased at the same mass, but merely increasing the power would be of no benefit in this case. However, one remaining alternative is to adjust the regulator of the heat exchanger more aggressively, although that would in turn result in even greater undershooting and overshooting. Rapid and precise temperature control would be impossible in this way.

Dynamic temperature regulation by means of a heat exchanger is also relatively inaccurate, i.e., if a constant temperature is not to be set. Apart from this, such a heat exchanger would necessitate additional parts and controllers for operating the heat exchanger, which would also make the plant more expensive.

DE 10 2010 046 946 A1 proposes controlling the temperature of the fuel in a conditioning plant by means of thermoelectric modules (so-called Peltier elements). Thus, because of the low storage masses achieved, a highly dynamic temperature regulation is possible, whereby the fuel can be both heated and cooled. This apparatus is also aimed specifically at conditioning liquid fuels.

There is the additional problem with gaseous fuels such as natural gas or hydrogen that the gaseous fuel is usually available or supplied, at a high pressure and consequently must first be depressurized to a lower pressure, which is required for use as a fuel in an internal combustion engine. However, when the gaseous fuel such as natural gas is depressurized, the fuel cools down drastically, which can be problematic for the downstream component of the conditioning plant, for example, due to the formation of condensate and ice on the gas lines or other components in the gas line. Therefore, the gaseous fuel is usually heated before being depressurized, so that the desired temperature of the fuel is achieved by decompression. Because of the fluctuations in pressure of the gaseous fuel supplied and also because of the dependence of temperature on the composition of the gaseous fuel after decompression, which can also vary, the temperature regulation of the gaseous fuel must be highly dynamic prior to decompression in order to be able to maintain a constant temperature after decompression and before the flow measurement. In addition the required heating power for temperature control of the fuel also depends greatly on the prevailing flow rate, which also necessitates a highly dynamic temperature regulation in the case of rapidly changing flow rates.

Such a highly dynamic temperature regulation necessitates, first of all, a regulating method that is capable of carrying out highly dynamic regulating intervention (in the sense of rapid changes in temperature), and secondly, a temperature control unit that is also capable of implementing the highly dynamic control intervention measures. Consequently, such a temperature control unit must be capable of implementing the required temperature changes in the flowing fuel within a very short period of time. In addition, a high thermal stability is also desired, also if under some circumstances high demands cannot be made of the dynamics of the temperature regulation because in certain applications a high precision and extremely constant regulation is required. These requirements necessitate a temperature control unit with a high heating and cooling power, but under some circumstances it may also be necessary to change rapidly between heating and cooling. Apart from this, an accurate temperature regulation must also be possible in order to prevent excessive overregulation of the temperature (either overheating or undercooling).

DE 10 2010 046 946 A1 gives the indication that for a highly dynamic temperature regulation, small thermal storage masses of the temperature control unit are advantageous.

U.S. Pat. No. 6,502,405 B1 discloses a heat exchanger element with Peltier elements for heating or cooling fuel in a vehicle. The heat exchanger element consists of a thermal conduction block in which a fuel line is installed in a meandering layout and which is insulated thermally on a first side. Peltier elements, which are thermally connected to a cooling body, are located on the second side of the thermal conduction block. The cooling body is typically designed with a large surface area and a small storage mass in order to maximize the heat dissipation capacity. In addition, a fan is also provided on the cooling body in order to further increase the capacity for dissipation of heat. Thus, the heat exchanger element of U.S. Pat. No. 6,502,405 B1 is also designed for a low thermal storage mass in order to be able to rapidly dissipate the heat to the surroundings via the cooling body. Due to the meandering layout of the fuel line in a heat exchanger element, however, there is also an uneven heating of the fuel, which makes the temperature regulation more difficult because all of the Peltier elements are controlled with the same power supply voltage. The uneven heating results in a higher temperature difference between the emission temperature of the medium and the surface of the Peltier elements, which in turn leads to a lower maximum emission temperature of the medium because the Peltier elements cannot be heated indefinitely. Or there is a lower maximum flow rate at a predetermined target emission temperature. Apart from this, more thermal energy is stored in the heat conducting block due to the greater temperature difference. This thermal energy must be dissipated again when there is a change in the target temperature, but that in turn makes the heat exchanger element more sluggish. For a more uniform heating of the fuel, the individual Peltier elements would either have to be coordinated with one another, i.e., different Peltier elements provided along the fuel line, or the Peltier elements would have to be supplied and regulated individually. However, both options would be very complicated and therefore a disadvantage.

However, the problems described above can basically occur with any gaseous or liquid medium whose temperature is to be regulated in a temperature control unit, not just with fuels.

Against the background of this prior art, it is an object of the present invention to provide a temperature control unit for a gaseous or liquid medium which permits a particularly highly dynamic and accurate temperature regulation of the medium.

This object is achieved according to the invention by selecting the mass ratio of the thermal storage mass of the cooling body to the thermal storage mass of the base body and the media line arranged therein to be in the range of 0.5 to 1, advantageously in the range of 0.7 to 0.8, and most especially advantageously to be 0.75.

It has been found that for a highly dynamic temperature regulation of a medium by means of a temperature control unit according to the preamble of claim 1, in particular when a rapid and repeated change in direction of heat flow is necessary, it is a disadvantage for the storage mass to be too low, as suggested by the state of the art. It has surprisingly been found that a certain mass ratio between the mass of the cooling body and the mass of the base body together with the media line arranged therein is advantageous for the regulation of temperature. The reason for this is apparently the fact that due to the greater mass of the cooling body, a thermal storage mass is formed and therefore thermal energy is not released to the environment too rapidly. This stored energy can then optionally be used for support in heating the fuel, so that the temperature control can be achieved more rapidly and with a greater precision.

A compact design of the temperature control unit is obtained when a groove into which the media line is pressed is provided in the base body.

For a very efficient temperature control, it is advantageous if the media line in the base body is arranged in a spiral pattern from the outside to the inside. Due to this arrangement of the media line in the base body in the form of a single-start spiral, a particularly uniform and efficient temperature control of the medium can be achieved. Due to the spiral shape, the temperature control unit may be designed very compactly because the spiral passes can be arranged close to one another. Therefore, a thermoelectric module may also cover multiple spiral passes, which improve the efficiency of the temperature control unit and the uniformity in heating. This makes it possible to achieve a particularly highly dynamic and accurate and stable temperature regulation of the medium.

Efficient temperature control is additionally supported when the multiple thermoelectric modules are arranged in multiple rows on the base body aligned around the periphery, wherein the module heating power of a thermoelectric module situated further toward the outside radially is greater than the module heating power of a thermoelectric module situated further toward the inside radially. In this way, the temperature of the medium flowing in from the outside can be regulated in the region of the higher heating power on the outside radially, which permits rapid and marked changes in temperature. The modules are then preferably coordinated with one another so that the temperature spread is minimal at the maximum flow rate between the module surface and the emission temperature of the medium. It has been found that this is the case when all the modules are at approximately the same surface temperature. Due to the peripheral arrangement, the thermoelectric modules within one row are naturally almost at the same temperature. Only the different rows would have to be balanced in this regard, which is a significant simplification in contrast to a meandering arrangement of the media line, because it is no longer necessary for all the thermoelectric modules to be balanced for the same result to be achieved (minimum temperature spread).

Furthermore, the module heating power can be optimally adapted to the conditions and modules having a lower module heating power can be installed on the inside radially.

To concentrate the thermal energy in the base body and to prevent an excessive drain of thermal energy, the base body is advantageously surrounded by a base body jacket wherein a plurality of radial connecting webs which are connected to the base body jacket are arranged over the circumference of the base body. This also increases the efficiency of the temperature control unit. This can be further improved if the base body jacket is designed to be partially hollow because this achieves even better thermal insulation between the base body and the surroundings.

It may be advantageous to arrange a cooling line in the cooling body through which cooling medium for cooling the cooling body flows as needed in order to be able to dissipate heat from the cooling body more rapidly. This may be useful in particular in the case of gases without a pronounced Joule-Thomson effect or with liquid media because in these cases, frequent reversal of polarity of the thermal modules may be necessary. The cooling line is then advantageously again arranged in a spiral.

The present invention is explained in greater detail below with reference to FIGS. 1 to 7, which illustrate advantageous embodiments of the invention as an example, schematically and without restriction, in which:

FIG. 1 shows a perspective view of the temperature control unit according to the invention,

FIG. 2 shows a view of a temperature control unit with the cooling body removed,

FIGS. 3 and 4 show views of the base body of a temperature control unit,

FIG. 5 shows a view of the media line in the temperature control unit,

FIG. 6 shows another advantageous arrangement of the media line in the base body, and

FIG. 7 shows a temperature control unit with a cooling line in the cooling body.

FIG. 1 shows a perspective view of the temperature control unit 1 according to the invention. The temperature control unit 1 consists of a base body 2 on which any fastening elements 3 may be provided for fastening the temperature control unit 1 such as, for example, feet in the exemplary embodiment shown here. On a first side of the base body 2, a thermal insulation element 4 is arranged and a cooling body 5 is arranged on the opposite second side. A media line 6 passes through the temperature control unit 1; a gaseous or liquid medium such as a fuel whose temperature is controlled at a desired level in the temperature control unit 1 flows through this media line 6. The media line 6 therefore has an input connection 10 and an output connection 11, so that the direction of flow of the medium through the temperature control unit 1 is defined (indicated by arrows in FIG. 1).

FIG. 2 shows the temperature control unit 1 with the cooling body 5 removed. A number of thermoelectric modules (Peltier elements) 7, which are arranged on the base body 2, can be seen therein. A thermoelectric module 7 is known to be a semiconductor element, which is arranged between a first heating surface 9 a (facing the base body 2 here, but not visible in FIG. 2) and a second heating surface 9 b (facing the cooling body 5 here). Depending on the polarity of the electric voltage supplied to the semiconductor element, either the first heating surface 9 a is hotter than the second heating surface 9 b or vice versa. Since the design and function of such thermoelectric modules 7 are sufficiently well known and such thermoelectric modules 7 are available commercially in various power classes, they will not be discussed in greater detail here.

Thus, depending on the polarity of the power supply voltage, which is supplied via terminals 8, for example, it is possible to provide both heating and cooling with such a thermoelectric module 7. “Heating” here means that heat is supplied to the base body 2, and “cooling” means that heat is withdrawn from the base body 2. The heat flow between the base body 2 and the cooling body 5 can thus be influenced with the thermoelectric modules 7.

The thermoelectric modules 7 are in thermodynamic contact with the base body 2 via a first heating surface 9 a (not visible in FIG. 2) directly or indirectly (for example, via a heat transfer element to improve the thermal conduction). The cooling body 5 is arranged on the second heating surface 9 b of the thermoelectric module and is in thermally conducting contact either directly or indirectly with the second hating surface 9 b. A cooling body 5 and the base body 2 are not arranged next to one another in order to prevent direct thermally conducting contact between the cooling body 5 and base body 2 (as can be seen in FIG. 1).

The base body 2 is illustrated in detail in FIGS. 3 and 4, which show the different views of the base body 2. FIG. 3 shows the side of the base body 2 on which the thermoelectric modules 7 are arranged. The base body 2 is made essentially of a base plate 20, which is surrounded along its circumference by a base body jacket 21. The base body jacket 21 is connected to the base plate 20 by radial connecting webs 22, wherein the connecting webs 22 are arranged so they are distributed around the circumference of the base plate 20. In the circumferential direction between the connecting webs 22, cavities 23 are formed, functioning as thermal insulation between the base plate 2 and the base body jacket 21. The heat flow from the base plate 20 into the base body jacket 21 is greatly reduced by the connecting webs 22 and the hollow spaces 23. Therefore, the heat introduced by the thermoelectric modules 7 into the base plate 20 remains concentrated there and flows only to a minor extent through the base body jacket 21 to the surroundings. This at the same time also achieves the goal that the base body jacket 21 and thus the temperature control unit 1 are not heated too greatly on the outside and that parasitic heat flows, which would reduce the power and dynamics of the conditioning, are minimized as much as possible.

The base body jacket 21 may additionally be designed to be hollow, in that peripheral slots 24 are incorporated into the base body jacket 21, also forming cavities for additional thermal insulation.

FIG. 4 shows the other side of the base body 2, where it can be seen that a groove 25, preferably a spiral groove into which the media line 6 is pressed in the assembled state, is formed on the backside of the base plate 20. The groove 25 here forms a single-start flat spiral (Archimedean spiral, logarithmic spiral) in the base body 2. The media line 6 is preferably guided in a spiral pattern from the outside to the inside, emerging from the temperature control unit 1 in the inner central region of the base plate 20, wherein the media line 6 is deflected, preferably by approx. 90°, out of the plane of the spiral on its exit from the unit in order to allow the media line 6 to easily emerge from the temperature control unit 1. Fundamentally, however, any other type of guidance of the media line 6 in the base body 20 is also conceivable.

The use of a media line 6 in the form of a single-start spiral is very complex from the standpoint of manufacturing technology because in this case the media line 6 extends in all three dimensions.

In an alternative embodiment, the media line 6 is arranged on the base body 2 in the form of a two-start planar spiral (also known as Fermat's parabolic spiral), as described with reference to FIG. 6. Again, a suitably shaped groove 25 to receive the media line 6 may be formed in the base body 2 for this purpose. The medium is supplied in a spiral pattern in the media line 6 from the outside radially to the inside centrally via a first spiral pass 27. On the inside centrally the first spiral pass 27 is connected to a second spiral pass 28 through which the medium is carried in the media line 6 from the inside radially to the outside radially in a spiral pattern. A first spiral pass 27 and a second spiral pass 28 are always situated radially side-by-side due to the two-start design of the groove 25. The medium is thus supplied on the outside radially through the input connection 10 and removed on the outside radially via the output connection 11. The two-start spiral has the advantage that the media line 6 need not be deflected out of the plane of the spiral, which is simple in terms of the manufacturing technology. The two-start spiral, however, has the disadvantage that the inflowing medium cools the medium flowing out, so somewhat more power is needed and the resulting heating achieved is less uniform. The temperature spread is therefore greater but the thermoelectric modules of one row will all still be at approximately the same temperature, in the case of coordinated modules.

The single-start or two-start spiral need not absolutely be designed as a circular spiral but instead may also have other shapes such as rectangular, square, etc. Due to the spiral shape the temperature control unit 1 may have a very compact design because the spiral passes can be arranged close to one another. Therefore, a great many running meters of medial line 6 can be accommodated in a small space, which increases the available surface for temperature control of the medium flowing through the media line 6.

To be able to implement a dense packing of the media line 6, bending radii must not come below minimum bending radii stipulated whilst shaping of the media line 6. A meandering layout of the media line would be a disadvantage in this regard because the required bending radii for a dense packing are considerably smaller than those with a spiral layout. With increasing pressure demands with regard to the media line 6, the minimum bending radius usually also increases because of the required increase in wall thickness. Therefore, a meandering layout has a particularly negative effect when there are high pressure demands, as in the present case.

FIG. 5 shows the thermal insulation element 4 with the media line 6, which is advantageously a spiral-shaped single-start line that is pressed into the base body 20 in the assembled state. Due to the thermal insulation element 4 this achieves the result that the heat introduced by the thermoelectric modules 7 into the base plate 20 remains concentrated there and is not discharged to the surroundings via the end face of the temperature control unit 1.

The thermoelectric modules 7 are preferably adapted in the form of a circle and/or adapted to the spiral form and arranged in multiple rows (that is at various radial distances) on the base plate 20 (FIG. 2). Therefore, more thermoelectric modules 7 may be arranged on the outside radially because of the resulting larger circumference. The inflowing medium is thus thermally regulated in the outer radial region where the heating power is higher, which permits marked and rapid changes in temperature. It is also advantageous if a thermoelectric module 7 which is arranged farther toward the inside radially has a lower module heating power than a thermoelectric module 7 arranged farther to the outside radially. Since the media line 6 is preferably guided to the inside in a single-start spiral, fewer and weaker (in the sense of less module heating power) thermoelectric modules on the inside radially are sufficient for temperature control on the medium. Thus, the temperature control of the medium can also be optimized by the arrangement and choice of the module heating power of the individual thermoelectric modules 7 and a very uniform heating of the medium can be achieved.

If an electric power supply voltage is applied to a thermoelectric module 7, then as is known one of the heating surfaces 9 a, 9 b of the thermoelectric module 7 is cooled off while at the same time the opposing heating surface 9 a, 9 b is heated. The maximum temperature spread between the heating surfaces 9 a, 9 b depends on the operating temperature (temperature on the warmer heating surface) of the thermoelectric module 7. The higher the operating temperature, the higher the maximum achievable temperature spread between the cold and hot heating surfaces 9 a, 9 b. Therefore, with the available thermoelectric modules 7, temperatures of up to 200° C. can be achieved on the hot heating surface, with the cold heating surface not exceeding 100° C. A highly dynamic regulation of the temperature is made possible by simply reversing the polarity of the power supply voltage. This regulation is supported in the temperature control unit 1 according to the invention, in that the cooling body 5 is used as a buffer storage in heating operation, i.e., when the medium in the media line 6 is to be heated. Therefore the thermal storage mass, however, should not be designed to be as small as possible as is suggested in the prior art, but instead a certain storage mass is desired in order to achieve this.

It has been found to be advantageous if the mass ratio of the thermal storage mass of the cooling body 5 to the thermal storage mass of the base body 2 and the media line 6 arranged therein is selected to be in the range of 0.5 to 1, advantageously 0.7 to 0.8. A most especially advantageous temperature regulability of the temperature control unit 1 was achieved at a mass ratio in the range of 0.75 and/or at a mass ratio of 0.75. A tested temperature control unit 1, for example, had a thermal storage mass of the cooling body 5 of 5.4 kg and a thermal storage mass of the base body 2 and the media line 6 arranged therein of 7.2 kg, which yields a mass ratio of 0.75.

In one embodiment as shown in FIG. 3 or FIG. 6, in which the base body jacket 21 is thermally separated from the base body 2 by means of cavities 23, the mass of the base body jacket 21 is not counted with the thermal storage mass of the base body. Likewise, the insulation element 4 is not part of the thermal storage mass of the base body 2.

At a constant heating demand of the temperature control unit 1, i.e., at a constant power supply voltage of the thermoelectric module 7, a stable temperature spread is established on the thermoelectric modules 7. As soon as less thermal energy and/or heat for temperature control of the medium is/are needed, the power supply voltage to the thermoelectric modules 7 is reduced so that the temperature spread also becomes lower. The temperature on the heating surface 9 a of the thermoelectric module 7, which is in contact with the base plate 20, therefore drops. At the same time, the temperature on the opposite heating surface 9 b rises. Thus there is a temperature gradient between the heating surface 9 b and the cooling body, which is adjacent to it so that heat flows into the cooling body 5 and is not dissipated to the surroundings immediately because of the thermal storage mass of the cooling body 5, but instead is stored temporarily (at least for a limited period of time). This temporarily stored thermal energy is available to the temperature regulation and/or temperature control unit 1 as support when more thermal energy is again needed for temperature control of the medium. In this case, the power supply voltage would be raised again so that the temperature spread on the thermoelectric modules 7 would increase again. The temperature on the heating surface 9 b with which the cooling body 5 is in contact would thus drop in comparison with the temperature of the cooling body 5. This results in an inverted temperature gradient, thus resulting in thermal energy (heat), which is stored in the cooling body 5, then flowing into the base body 2 and thus supporting the thermoelectric modules 7. Because of the thermal storage mass of the cooling body 5, it is possible for the temperature control unit 1 to respond very rapidly and accurately to load alternations and/or changes in temperature, and the typical excess temperature control is can be prevented to the greatest extent. However, this requires the thermal storage mass of the cooling body 5 to be not too large or too small in comparison with the thermal storage mass of the base body 2 and the media line 6 arranged therein.

The total surface area of the cooling body 5 should be designed as a function of the operating temperature to be expected, so that the heat stored in the cooling body 5 is not released too rapidly to the surface but instead remains stored in the cooling body 5 for a sufficient period of time. The surface is therefore not to be dimensioned to be as large as possible and optimized for the dissipation of heat, as it would be in a traditional cooling body, but on the contrary, it is to be dimensioned so that the heat remains stored in the cooling body 5.

Complete thermal insulation of the cooling body 5 from the surroundings would also be a disadvantage because in the case of frequent reversals of polarity, the temperature in the cooling body 5 might escalate.

For various media, the material of the media line 6 and the heating power of the thermoelectric module 7 may optionally be adapted. However, the general basic principle with the cooling body 5 as a storage mass for support of the temperature control unit 1 remains unaffected.

For certain gaseous media such as natural gas, there is a great cooling in accordance with the Joule-Thomson effect due to the required depressurization. With these gases the temperature control unit 1 must usually only preheat the gaseous medium. Cooling of these gases by the temperature control unit 1 is usually not necessary. Therefore, it is normally also sufficient for these applications to work only with the temperature spread of the thermoelectric module 7. Reversal of the polarity to switch from heating to cooling is rather not necessary.

Other gaseous media such as hydrogen do not have this pronounced effect of extreme cooling due to the required depressurization. On the contrary, there may even be a heating due to depressurization. In temperature control of liquid media, often no depressurization is necessary because the liquid medium is already at the correct pressure.

In the case of gases without a pronounced Joule-Thomson effect or with liquid media, the temperature control unit 1 therefore must often switch between heating and cooling the gaseous medium in order to keep the temperature constant as a function of the pressure and the flow rate. In particular in the case of cooling, however, it may happen that because of the lower surface area of the cooling body 5, the heat formed, in particular the waste heat of the thermoelectric modules 7, cannot be dissipated rapidly enough. Therefore, when using temperature control unit 1 with such gaseous or liquid media, provisions may also be taken to additionally cool the cooling body 5 as needed. Therefore, a cooling line 12 may be introduced into the cooling body 5. The cooling liquid is sent through this line for the additional cooling of the cooling body 5. Such a design is indicated in FIG. 7. The cooling line 12 may again be arranged in the cooling body 5 in the form of a single-start or two-start spiral as described above with respect to the media line 6. Therefore, the cooling body 5 may also be designed in multiple parts in order to be able to introduce the cooling line 12. However, other embodiments of the cooling line 12 are of course also conceivable.

In the exemplary embodiment shown in FIG. 7, grooves 31 are cut into a cooling body base body 30, for example by milling, in order to form the cooling line 12. The grooves 31 are preferably cut in the form of spirals as described above. The cooling body base body 30 with the grooves 31 is covered with a cooling body cover 32 in order to form the cooling body 5.

If a separate line is used as cooling line 12 in the cooling body 5 (like the media line 6 in the base body), then the cooling line 12 would also be part of the thermal storage mass of the cooling body 5.

To be able to connect the cooling line 12 in the cooling body 5, a cooling medium supply connection 34 and a cooling medium removal connection 33 may be provided on the cooling body. The cooling medium is preferably supplied from the inside and removed centrally on the outside. 

1. A temperature control unit for temperature control of a gaseous or liquid medium by means of a number of thermoelectric modules, which are arranged between a base body and a cooling body, and a media line through which the gaseous or liquid medium flows is arranged in the base body, wherein the mass ratio of the thermal storage mass of the cooling body to the thermal storage mass of the base body and the media line arranged therein is in the range of 0.5 to 1, advantageously in the range of 0.7 to 0.8.
 2. The temperature control unit according to claim 1, wherein the mass ratio is 0.75.
 3. The temperature control unit according to claim 1, wherein a groove into which the media line is pressed is provided in the base body.
 4. The temperature control unit according to claim 3, wherein the media line is arranged in the base body in the form of a spiral leading from the outside to the inside.
 5. The temperature control unit according to claim 3, wherein the media line is arranged in the base body in the form of a two-start spiral in a first spiral start leading from the outside to the inside and in a second spiral start connected radially at the inside to the first spiral start leading from the inside to the outside.
 6. The temperature control unit according to claim 5, wherein the multiple thermoelectric modules are arranged in a plurality of rows on the base body wherein the module heating power of a thermoelectric module situated further toward the outside radially is greater than the module heating power of a thermoelectric module situated further toward the inside radially.
 7. The temperature control unit according to claim 1, wherein the base body is surrounded by a base body jacket wherein a plurality of radial connecting webs which are connected to the base body jacket are arranged over the circumference of the base body.
 8. The temperature control unit according to claim 7, wherein the base body jacket is designed to be partially hollow.
 9. The temperature control unit according to claim 1, wherein a cooling line through which cooling medium for cooling the cooling body flows as needed is arranged in the cooling body.
 10. The temperature control unit according to claim 9, wherein the cooling line is arranged in the form of a spiral.
 11. The temperature control unit according to claim 1, wherein the media line is arranged in the base body in the form of a spiral leading from the outside to the inside.
 12. The temperature control unit according to claim 1, wherein the media line is arranged in the base body in the form of a two-start spiral in a first spiral start leading from the outside to the inside and in a second spiral start connected radially at the inside to the first spiral start leading from the inside to the outside.
 13. The temperature control unit according to claim 4, wherein the multiple thermoelectric modules are arranged in a plurality of rows on the base body wherein the module heating power of a thermoelectric module situated further toward the outside radially is greater than the module heating power of a thermoelectric module situated further toward the inside radially. 